{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:EWUGMGSO3ALK2UQFAP3T7EVMVE","short_pith_number":"pith:EWUGMGSO","schema_version":"1.0","canonical_sha256":"25a8661a4ed816ad520503f73f92aca91697dd96ebf9d32b0e81ec44de5e1835","source":{"kind":"arxiv","id":"hep-lat/0502003","version":1},"attestation_state":"computed","paper":{"title":"Properties of the deconfining phase transition in SU(N) gauge theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"B. Lucini, M. Teper, U. Wenger","submitted_at":"2005-02-03T15:52:02Z","abstract_excerpt":"We extend our earlier investigation of the finite temperature deconfinement transition in SU(N) gauge theories, with the emphasis on what happens as N->oo. We calculate the latent heat in the continuum limit, and find the expected quadratic in N behaviour at large N. We confirm that the phase transition, which is second order for SU(2) and weakly first order for SU(3), becomes robustly first order for N>3 and strengthens as N increases. As an aside, we explain why the SU(2) specific heat shows no sign of any peak as T is varied across what is supposedly a second order phase transition. We calc"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-lat/0502003","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-02-03T15:52:02Z","cross_cats_sorted":[],"title_canon_sha256":"b67eb06483a281b6edb5bde78215055b892da1263c147f33959abce993def391","abstract_canon_sha256":"819eaa8d71081ebc62a293f6f2b372d87ff1e8ad57448b5fd412598de105372a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:20:18.953083Z","signature_b64":"XufkheFIdPM89pZi7FBpnt7clnfWcJljMvgxsnASm7Y31BqlLCrrqGLxagA+t1FB5Khdmx0ax929xz6BGbXtCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"25a8661a4ed816ad520503f73f92aca91697dd96ebf9d32b0e81ec44de5e1835","last_reissued_at":"2026-07-04T15:20:18.952736Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:20:18.952736Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Properties of the deconfining phase transition in SU(N) gauge theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"B. Lucini, M. Teper, U. Wenger","submitted_at":"2005-02-03T15:52:02Z","abstract_excerpt":"We extend our earlier investigation of the finite temperature deconfinement transition in SU(N) gauge theories, with the emphasis on what happens as N->oo. We calculate the latent heat in the continuum limit, and find the expected quadratic in N behaviour at large N. We confirm that the phase transition, which is second order for SU(2) and weakly first order for SU(3), becomes robustly first order for N>3 and strengthens as N increases. As an aside, we explain why the SU(2) specific heat shows no sign of any peak as T is varied across what is supposedly a second order phase transition. We calc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0502003","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/0502003/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0502003","created_at":"2026-07-04T15:20:18.952797+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0502003v1","created_at":"2026-07-04T15:20:18.952797+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0502003","created_at":"2026-07-04T15:20:18.952797+00:00"},{"alias_kind":"pith_short_12","alias_value":"EWUGMGSO3ALK","created_at":"2026-07-04T15:20:18.952797+00:00"},{"alias_kind":"pith_short_16","alias_value":"EWUGMGSO3ALK2UQF","created_at":"2026-07-04T15:20:18.952797+00:00"},{"alias_kind":"pith_short_8","alias_value":"EWUGMGSO","created_at":"2026-07-04T15:20:18.952797+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2606.30760","citing_title":"Rich Phenomenology from Simple Ingredients: A Review of Confining Dark Sectors","ref_index":202,"is_internal_anchor":true},{"citing_arxiv_id":"2508.07919","citing_title":"Topological Strings in SU(3) Gauge Theory at Finite Temperature","ref_index":29,"is_internal_anchor":true},{"citing_arxiv_id":"2509.19009","citing_title":"Finite-temperature Yang-Mills theories with the density of states method: towards the continuum limit","ref_index":25,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EWUGMGSO3ALK2UQFAP3T7EVMVE","json":"https://pith.science/pith/EWUGMGSO3ALK2UQFAP3T7EVMVE.json","graph_json":"https://pith.science/api/pith-number/EWUGMGSO3ALK2UQFAP3T7EVMVE/graph.json","events_json":"https://pith.science/api/pith-number/EWUGMGSO3ALK2UQFAP3T7EVMVE/events.json","paper":"https://pith.science/paper/EWUGMGSO"},"agent_actions":{"view_html":"https://pith.science/pith/EWUGMGSO3ALK2UQFAP3T7EVMVE","download_json":"https://pith.science/pith/EWUGMGSO3ALK2UQFAP3T7EVMVE.json","view_paper":"https://pith.science/paper/EWUGMGSO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0502003&json=true","fetch_graph":"https://pith.science/api/pith-number/EWUGMGSO3ALK2UQFAP3T7EVMVE/graph.json","fetch_events":"https://pith.science/api/pith-number/EWUGMGSO3ALK2UQFAP3T7EVMVE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EWUGMGSO3ALK2UQFAP3T7EVMVE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EWUGMGSO3ALK2UQFAP3T7EVMVE/action/storage_attestation","attest_author":"https://pith.science/pith/EWUGMGSO3ALK2UQFAP3T7EVMVE/action/author_attestation","sign_citation":"https://pith.science/pith/EWUGMGSO3ALK2UQFAP3T7EVMVE/action/citation_signature","submit_replication":"https://pith.science/pith/EWUGMGSO3ALK2UQFAP3T7EVMVE/action/replication_record"}},"created_at":"2026-07-04T15:20:18.952797+00:00","updated_at":"2026-07-04T15:20:18.952797+00:00"}